organic compounds
4-Hydroxy-3-methoxybenzaldehyde thiosemicarbazone
aDepartamento de Química, Universidade Federal de Sergipe, Av. Marechal Rondon s/n, Campus, 49100-000 São Cristóvão–SE, Brazil, and bInstitut für Anorganische Chemie, Christian-Albrechts-Universität zu Kiel, Max-Eyth Strasse 2, D-24118 Kiel, Germany
*Correspondence e-mail: adriano@daad-alumni.de
In the title compound, C9H11N3S, there is an intramolecular O—H⋯O hydrogen bond involving the OH group and the adjacent methoxy O atom. The molecule is essentially planar, with the maximum deviation from the mean plane of the non-H atoms being 0.1127 (14) Å for the methyl C atom. In the crystal, molecules are connected via centrosymmetric pairs of N—H⋯S and O—H⋯O hydrogen bonds into a two-dimensional network parallel to (10-3).
CCDC reference: 973962
Related literature
For the in vitro antimalarial and antitubercular activity of hydroxy-methoxybenzaldehyde thiosemicarbazone derivatives, see: Khanye et al. (2011). For the first report of the synthesis, see: Freund & Schander (1902). For the synthesis and of an isomer of the title compound, see: Hao (2010).
Experimental
Crystal data
|
Data collection: X-AREA (Stoe & Cie, 2008); cell X-AREA; data reduction: X-RED32 (Stoe & Cie, 2008); program(s) used to solve structure: SHELXS97 (Sheldrick, 2008); program(s) used to refine structure: SHELXL97 (Sheldrick, 2008); molecular graphics: DIAMOND (Brandenburg, 2006); software used to prepare material for publication: publCIF (Westrip, 2010).
Supporting information
CCDC reference: 973962
10.1107/S1600536813032303/fy2108sup1.cif
contains datablock I. DOI:Structure factors: contains datablock I. DOI: 10.1107/S1600536813032303/fy2108Isup2.hkl
Supporting information file. DOI: 10.1107/S1600536813032303/fy2108Isup3.cml
The starting materials were commercially available and were used without further purification. The 4-hydroxy-3-methoxybenzaldehyde thiosemicarbazone synthesis was adapted from a procedure reported previously (Freund & Schander, 1902). The hydrochloric acid catalyzed reaction of vanillin (8.83 mmol) and thiosemicarbazide (8.83 mmol) in ethanol (50 ml) was refluxed for 6 h. After cooling and filtering, the title compound was obtained. Crystals suitable for X-ray diffraction were obtained from the reaction mixture by the slow evaporation of solvent.
All H atoms were were positioned with idealized geometry (methyl and O—H H atoms allowed to rotate but not to tip) and were refined as isotropic with Uiso(H) = 1.2 or 1.5 Ueq(C, N and O) using a riding model with C—H = 0.95 Å for aromatic H atoms, C—H = 0.98 for methyl H atoms, N—H = 0.88 Å for amine and hydrazine H atoms and O—H = 0.84 Å for the O—H H atom.
Data collection: X-AREA (Stoe & Cie, 2008); cell
X-AREA (Stoe & Cie, 2008); data reduction: X-RED32 (Stoe & Cie, 2008); program(s) used to solve structure: SHELXS97 (Sheldrick, 2008); program(s) used to refine structure: SHELXL97 (Sheldrick, 2008); molecular graphics: DIAMOND (Brandenburg, 2006); software used to prepare material for publication: publCIF (Westrip, 2010).Fig. 1. Molecular structure of the title compound with labeling and displacement ellipsoids drawn at the 70% probability level. | |
Fig. 2. Crystal structure of the title compound with hydrogen bonds shown as dashed lines. |
C9H11N3O2S | Z = 2 |
Mr = 225.27 | F(000) = 236 |
Triclinic, P1 | Dx = 1.447 Mg m−3 |
Hall symbol: -P 1 | Mo Kα radiation, λ = 0.71073 Å |
a = 4.5886 (5) Å | Cell parameters from 5179 reflections |
b = 8.5213 (11) Å | θ = 2.5–27.0° |
c = 13.9621 (15) Å | µ = 0.30 mm−1 |
α = 75.898 (13)° | T = 200 K |
β = 87.669 (13)° | Block, yellow |
γ = 77.580 (14)° | 0.4 × 0.3 × 0.2 mm |
V = 517.05 (10) Å3 |
Stoe IPDS-1 diffractometer | 2211 independent reflections |
Radiation source: fine-focus sealed tube, Stoe IPDS-1 | 1829 reflections with I > 2σ(I) |
Graphite monochromator | Rint = 0.040 |
ϕ scans | θmax = 27.0°, θmin = 2.5° |
Absorption correction: numerical (X-SHAPE and X-RED32; Stoe & Cie, 2008) | h = −5→5 |
Tmin = 0.865, Tmax = 0.982 | k = −10→10 |
5179 measured reflections | l = −17→17 |
Refinement on F2 | Secondary atom site location: difference Fourier map |
Least-squares matrix: full | Hydrogen site location: inferred from neighbouring sites |
R[F2 > 2σ(F2)] = 0.036 | H-atom parameters constrained |
wR(F2) = 0.100 | w = 1/[σ2(Fo2) + (0.0666P)2] where P = (Fo2 + 2Fc2)/3 |
S = 1.03 | (Δ/σ)max = 0.001 |
2211 reflections | Δρmax = 0.32 e Å−3 |
139 parameters | Δρmin = −0.27 e Å−3 |
0 restraints | Extinction correction: SHELXL97 (Sheldrick, 2008), Fc*=kFc[1+0.001xFc2λ3/sin(2θ)]-1/4 |
Primary atom site location: structure-invariant direct methods | Extinction coefficient: 0.055 (15) |
C9H11N3O2S | γ = 77.580 (14)° |
Mr = 225.27 | V = 517.05 (10) Å3 |
Triclinic, P1 | Z = 2 |
a = 4.5886 (5) Å | Mo Kα radiation |
b = 8.5213 (11) Å | µ = 0.30 mm−1 |
c = 13.9621 (15) Å | T = 200 K |
α = 75.898 (13)° | 0.4 × 0.3 × 0.2 mm |
β = 87.669 (13)° |
Stoe IPDS-1 diffractometer | 2211 independent reflections |
Absorption correction: numerical (X-SHAPE and X-RED32; Stoe & Cie, 2008) | 1829 reflections with I > 2σ(I) |
Tmin = 0.865, Tmax = 0.982 | Rint = 0.040 |
5179 measured reflections |
R[F2 > 2σ(F2)] = 0.036 | 0 restraints |
wR(F2) = 0.100 | H-atom parameters constrained |
S = 1.03 | Δρmax = 0.32 e Å−3 |
2211 reflections | Δρmin = −0.27 e Å−3 |
139 parameters |
Geometry. All e.s.d.'s (except the e.s.d. in the dihedral angle between two l.s. planes) are estimated using the full covariance matrix. The cell e.s.d.'s are taken into account individually in the estimation of e.s.d.'s in distances, angles and torsion angles; correlations between e.s.d.'s in cell parameters are only used when they are defined by crystal symmetry. An approximate (isotropic) treatment of cell e.s.d.'s is used for estimating e.s.d.'s involving l.s. planes. |
Refinement. Refinement of F2 against ALL reflections. The weighted R-factor wR and goodness of fit S are based on F2, conventional R-factors R are based on F, with F set to zero for negative F2. The threshold expression of F2 > σ(F2) is used only for calculating R-factors(gt) etc. and is not relevant to the choice of reflections for refinement. R-factors based on F2 are statistically about twice as large as those based on F, and R- factors based on ALL data will be even larger. |
x | y | z | Uiso*/Ueq | ||
C1 | 0.1779 (3) | 0.65909 (18) | 0.22576 (11) | 0.0210 (3) | |
C2 | 0.0643 (3) | 0.81737 (19) | 0.16881 (12) | 0.0252 (3) | |
H2 | 0.1261 | 0.9096 | 0.1820 | 0.030* | |
C3 | −0.1384 (4) | 0.84153 (19) | 0.09296 (12) | 0.0255 (3) | |
H3 | −0.2163 | 0.9501 | 0.0546 | 0.031* | |
C4 | −0.2278 (3) | 0.70678 (19) | 0.07295 (11) | 0.0223 (3) | |
C5 | −0.1165 (3) | 0.54775 (17) | 0.12986 (11) | 0.0203 (3) | |
C6 | 0.0858 (3) | 0.52373 (18) | 0.20585 (11) | 0.0207 (3) | |
H6 | 0.1622 | 0.4152 | 0.2445 | 0.025* | |
O1 | −0.4253 (3) | 0.73483 (14) | −0.00291 (9) | 0.0306 (3) | |
H1 | −0.4773 | 0.6463 | −0.0034 | 0.046* | |
O2 | −0.2264 (3) | 0.42408 (13) | 0.10546 (8) | 0.0268 (3) | |
C7 | −0.1404 (4) | 0.2626 (2) | 0.16928 (14) | 0.0354 (4) | |
H7A | 0.0761 | 0.2238 | 0.1664 | 0.053* | |
H7B | −0.2414 | 0.1863 | 0.1481 | 0.053* | |
H7C | −0.1969 | 0.2671 | 0.2372 | 0.053* | |
C8 | 0.3893 (3) | 0.62554 (19) | 0.30740 (11) | 0.0218 (3) | |
H8 | 0.4565 | 0.5145 | 0.3439 | 0.026* | |
N1 | 0.4870 (3) | 0.74084 (16) | 0.33129 (9) | 0.0222 (3) | |
N2 | 0.6853 (3) | 0.68715 (15) | 0.40998 (10) | 0.0222 (3) | |
H2A | 0.7455 | 0.5805 | 0.4362 | 0.027* | |
C9 | 0.7865 (3) | 0.79732 (18) | 0.44648 (11) | 0.0218 (3) | |
N3 | 0.6948 (4) | 0.95590 (17) | 0.40253 (11) | 0.0344 (4) | |
H3A | 0.5720 | 0.9854 | 0.3514 | 0.041* | |
H3B | 0.7565 | 1.0318 | 0.4244 | 0.041* | |
S1 | 1.01872 (9) | 0.72984 (5) | 0.54636 (3) | 0.02745 (16) |
U11 | U22 | U33 | U12 | U13 | U23 | |
C1 | 0.0178 (7) | 0.0265 (7) | 0.0203 (7) | −0.0054 (6) | −0.0038 (5) | −0.0074 (6) |
C2 | 0.0253 (8) | 0.0239 (7) | 0.0286 (8) | −0.0074 (6) | −0.0071 (6) | −0.0074 (6) |
C3 | 0.0270 (8) | 0.0216 (7) | 0.0265 (8) | −0.0051 (6) | −0.0080 (6) | −0.0015 (6) |
C4 | 0.0207 (7) | 0.0270 (7) | 0.0193 (7) | −0.0040 (6) | −0.0073 (6) | −0.0054 (6) |
C5 | 0.0203 (7) | 0.0223 (7) | 0.0208 (7) | −0.0055 (6) | −0.0027 (5) | −0.0085 (6) |
C6 | 0.0203 (7) | 0.0229 (7) | 0.0193 (7) | −0.0041 (6) | −0.0040 (6) | −0.0054 (6) |
O1 | 0.0350 (6) | 0.0285 (6) | 0.0283 (6) | −0.0066 (5) | −0.0196 (5) | −0.0035 (5) |
O2 | 0.0334 (6) | 0.0224 (5) | 0.0266 (6) | −0.0065 (4) | −0.0144 (5) | −0.0064 (4) |
C7 | 0.0458 (10) | 0.0233 (8) | 0.0377 (10) | −0.0093 (7) | −0.0219 (8) | −0.0031 (7) |
C8 | 0.0192 (7) | 0.0261 (7) | 0.0212 (7) | −0.0049 (5) | −0.0050 (6) | −0.0070 (6) |
N1 | 0.0197 (6) | 0.0278 (6) | 0.0204 (6) | −0.0038 (5) | −0.0070 (5) | −0.0078 (5) |
N2 | 0.0232 (6) | 0.0224 (6) | 0.0224 (7) | −0.0045 (5) | −0.0095 (5) | −0.0068 (5) |
C9 | 0.0210 (7) | 0.0247 (7) | 0.0217 (7) | −0.0060 (6) | −0.0020 (6) | −0.0080 (6) |
N3 | 0.0470 (9) | 0.0227 (7) | 0.0346 (8) | −0.0065 (6) | −0.0228 (7) | −0.0059 (6) |
S1 | 0.0345 (3) | 0.0250 (2) | 0.0248 (2) | −0.00760 (16) | −0.01444 (16) | −0.00630 (15) |
C1—C2 | 1.390 (2) | O2—C7 | 1.428 (2) |
C1—C6 | 1.401 (2) | C7—H7A | 0.9800 |
C1—C8 | 1.4608 (19) | C7—H7B | 0.9800 |
C2—C3 | 1.386 (2) | C7—H7C | 0.9800 |
C2—H2 | 0.9500 | C8—N1 | 1.2801 (19) |
C3—C4 | 1.390 (2) | C8—H8 | 0.9500 |
C3—H3 | 0.9500 | N1—N2 | 1.3792 (17) |
C4—O1 | 1.3643 (17) | N2—C9 | 1.3404 (19) |
C4—C5 | 1.393 (2) | N2—H2A | 0.8800 |
C5—O2 | 1.3779 (17) | C9—N3 | 1.324 (2) |
C5—C6 | 1.386 (2) | C9—S1 | 1.6962 (15) |
C6—H6 | 0.9500 | N3—H3A | 0.8800 |
O1—H1 | 0.8400 | N3—H3B | 0.8800 |
C2—C1—C6 | 119.42 (13) | O2—C7—H7A | 109.5 |
C2—C1—C8 | 123.13 (13) | O2—C7—H7B | 109.5 |
C6—C1—C8 | 117.45 (13) | H7A—C7—H7B | 109.5 |
C3—C2—C1 | 120.45 (13) | O2—C7—H7C | 109.5 |
C3—C2—H2 | 119.8 | H7A—C7—H7C | 109.5 |
C1—C2—H2 | 119.8 | H7B—C7—H7C | 109.5 |
C2—C3—C4 | 119.99 (14) | N1—C8—C1 | 122.15 (14) |
C2—C3—H3 | 120.0 | N1—C8—H8 | 118.9 |
C4—C3—H3 | 120.0 | C1—C8—H8 | 118.9 |
O1—C4—C3 | 118.45 (13) | C8—N1—N2 | 114.48 (12) |
O1—C4—C5 | 121.52 (13) | C9—N2—N1 | 120.04 (12) |
C3—C4—C5 | 120.02 (13) | C9—N2—H2A | 120.0 |
O2—C5—C6 | 124.88 (13) | N1—N2—H2A | 120.0 |
O2—C5—C4 | 115.17 (13) | N3—C9—N2 | 117.44 (14) |
C6—C5—C4 | 119.95 (13) | N3—C9—S1 | 123.06 (11) |
C5—C6—C1 | 120.17 (14) | N2—C9—S1 | 119.49 (11) |
C5—C6—H6 | 119.9 | C9—N3—H3A | 120.0 |
C1—C6—H6 | 119.9 | C9—N3—H3B | 120.0 |
C4—O1—H1 | 109.5 | H3A—N3—H3B | 120.0 |
C5—O2—C7 | 116.19 (11) | ||
C6—C1—C2—C3 | 0.1 (2) | C2—C1—C6—C5 | 0.1 (2) |
C8—C1—C2—C3 | −179.27 (15) | C8—C1—C6—C5 | 179.45 (13) |
C1—C2—C3—C4 | −0.5 (3) | C6—C5—O2—C7 | 5.2 (2) |
C2—C3—C4—O1 | −179.32 (15) | C4—C5—O2—C7 | −173.55 (15) |
C2—C3—C4—C5 | 0.8 (3) | C2—C1—C8—N1 | −0.7 (2) |
O1—C4—C5—O2 | −1.7 (2) | C6—C1—C8—N1 | 179.91 (14) |
C3—C4—C5—O2 | 178.21 (14) | C1—C8—N1—N2 | −179.89 (13) |
O1—C4—C5—C6 | 179.46 (14) | C8—N1—N2—C9 | −175.18 (14) |
C3—C4—C5—C6 | −0.6 (2) | N1—N2—C9—N3 | −1.7 (2) |
O2—C5—C6—C1 | −178.53 (14) | N1—N2—C9—S1 | 177.37 (11) |
C4—C5—C6—C1 | 0.2 (2) |
D—H···A | D—H | H···A | D···A | D—H···A |
O1—H1···O2 | 0.84 | 2.24 | 2.6934 (16) | 114 |
O1—H1···O2i | 0.84 | 2.27 | 2.9153 (15) | 134 |
N2—H2A···S1ii | 0.88 | 2.59 | 3.4319 (14) | 161 |
N3—H3B···S1iii | 0.88 | 2.59 | 3.4540 (15) | 169 |
Symmetry codes: (i) −x−1, −y+1, −z; (ii) −x+2, −y+1, −z+1; (iii) −x+2, −y+2, −z+1. |
D—H···A | D—H | H···A | D···A | D—H···A |
O1—H1···O2 | 0.84 | 2.24 | 2.6934 (16) | 113.9 |
O1—H1···O2i | 0.84 | 2.27 | 2.9153 (15) | 133.5 |
N2—H2A···S1ii | 0.88 | 2.59 | 3.4319 (14) | 160.8 |
N3—H3B···S1iii | 0.88 | 2.59 | 3.4540 (15) | 168.5 |
Symmetry codes: (i) −x−1, −y+1, −z; (ii) −x+2, −y+1, −z+1; (iii) −x+2, −y+2, −z+1. |
Acknowledgements
We gratefully acknowledge financial support by the State of Schleswig–Holstein, Germany. We thank Professor Dr Wolfgang Bensch for access to his experimental facilities. BRSF thanks CNPq/UFS for the award of a PIBIC scholarship and ABO acknowledges financial support through the FAPITEC/SE/FUNTEC/CNPq PPP 04/2011 program.
References
Brandenburg, K. (2006). DIAMOND. Crystal Impact GbR, Bonn, Germany. Google Scholar
Freund, M. & Schander, A. (1902). Chem. Ber. 35, 2602–2606. CrossRef CAS Google Scholar
Hao, Y.-M. (2010). Acta Cryst. E66, o2211. Web of Science CSD CrossRef IUCr Journals Google Scholar
Khanye, S. D., Wan, B., Franzblau, S. G., Gut, J., Rosenthal, P. J., Smith, G. S. & Chibale, K. (2011). J. Organomet. Chem. 696, 3392–3396. Web of Science CrossRef CAS Google Scholar
Sheldrick, G. M. (2008). Acta Cryst. A64, 112–122. Web of Science CrossRef CAS IUCr Journals Google Scholar
Stoe & Cie (2008). X-AREA, X-RED32 and X-SHAPE. Stoe & Cie, Darmstadt, Germany. Google Scholar
Westrip, S. P. (2010). J. Appl. Cryst. 43, 920–925. Web of Science CrossRef CAS IUCr Journals Google Scholar
This is an open-access article distributed under the terms of the Creative Commons Attribution (CC-BY) Licence, which permits unrestricted use, distribution, and reproduction in any medium, provided the original authors and source are cited.
Thiosemicarbazone derivatives have a wide range of pharmacological properties. For example, benzaldehyde-thiosemicarbazone derivatives show in vitro antimalarial and antitubercular activity (Khanye et al., 2011). As part of our study on the synthesis of thiosemicarbazone derivatives, we report herein the crystal structure of 4-hydroxy-3-methoxybenzaldehyde thiosemicarbazone. In the title compound (Fig. 1), in which the molecular structure matches the asymmetric unit, the maximal deviation from the least squares plane through all non-hydrogen atoms amount to 0.1127 (14) Å for C7. The molecule shows a trans conformation for the atoms about the C8—N1/N1—N2/N2—C9/ bonds. This conformation is also observed in the literature for an isomer of the title compound (Hao, 2010). The mean deviations from the least squares planes for the C1—C8/O1—O2 and C9/N1—N3/S1 fragments amount to 0.0733 (12) Å for C7 and 0.0188 (10) Å for N2, respectively, and the dihedral angle between the two planes is 5.08 (6)°.
The molecules are connected via centrosymmetric pairs of N—H···S and O—H···O hydrogen interactions, forming a two-dimensional H-bonded polymer. An O—H···O intramolecular H-interaction is also observed (Fig. 2 and Table 1). The molecules are arranged in layers, stacked along the a-axis direction through π–π-interactions, with the shortest C···C distance being 3.380 (23) Å [C8···C5iv, (iv): 1+x, y, z].